CN108169208A - A kind of Raman spectrum detector calibration method - Google Patents
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Abstract
一种拉曼光谱检测仪校准方法,包括以下操作步骤,步骤一,得到参考光谱S1;步骤二,得到初始光谱S2;步骤三,得到当前背景光谱S3;步骤四,计算所述参考光谱S1与所述初始光谱S2的第一差值光谱Sd1,计算所述参考光谱S1与当前背景光谱S3的第二差值光谱Sd2,计算所述初始光谱S2与所述当前背景光谱S3的第三差值光谱Sd3;步骤五,确定第一偏移量△v1与第二偏移量△v2;步骤六,采用所述第一偏移量△v1对检测结果的拉曼光谱进行修正或采用所述第四偏移量△v4对检测结果的拉曼光谱进行修正。本发明拥有校准参照多,校准度高,实时性好的优点。
A method for calibrating a Raman spectrometer, comprising the following steps: Step 1, obtain a reference spectrum S1; Step 2, obtain an initial spectrum S2; Step 3, obtain a current background spectrum S3; Step 4, calculate the reference spectrum S1 and The first difference spectrum Sd1 of the initial spectrum S2, calculate the second difference spectrum Sd2 between the reference spectrum S1 and the current background spectrum S3, and calculate the third difference between the initial spectrum S2 and the current background spectrum S3 Spectrum Sd3; Step 5, determine the first offset Δv1 and the second offset Δv2; Step 6, use the first offset Δv1 to correct the Raman spectrum of the detection result or use the first offset Δv1 The four offsets △v4 correct the Raman spectrum of the detection result. The invention has the advantages of many calibration references, high calibration degree and good real-time performance.
Description
技术领域technical field
本发明涉及拉曼光谱检测技术领域,具体涉及一种拉曼光谱检测仪校准方法。The invention relates to the technical field of Raman spectrum detection, in particular to a method for calibrating a Raman spectrum detector.
背景技术Background technique
拉曼光谱仪的激光的波长通常是在激光器出厂时或是拉曼光谱仪出厂时进行标定测量已确定。但是激光的波长会因为环境温度、电子电路的波动等发生微小的漂移。应用在拉曼光谱仪上的激光器通常对激光波长的稳定性要求较高,要求±2cm-1或更高,其稳定性参数直接影响仪器的拉曼偏移测量精度。拉曼光谱仪出厂后在长期使用、环境变化、长途运输后等其激光波长均有可能发生漂移,通常会通过自校准等方式对激光波长进行修正。通常的自校准方法是:测量某种标准物质(如聚苯乙烯)的拉曼光谱,并与该标准物质的标准谱图进行对比,进而得知激光波长的偏移量。现有的自校准的方法的缺点在于,其不具备实时性,只能给定一个恒定的修正值,且什么状态下进行自校准的条件难于把握。The wavelength of the laser of the Raman spectrometer is usually determined by calibration measurement when the laser leaves the factory or when the Raman spectrometer leaves the factory. However, the wavelength of the laser will drift slightly due to ambient temperature and fluctuations in electronic circuits. Lasers used in Raman spectrometers usually have high requirements on the stability of the laser wavelength, requiring ±2cm-1 or higher, and its stability parameters directly affect the Raman shift measurement accuracy of the instrument. After the Raman spectrometer leaves the factory, the laser wavelength may drift after long-term use, environmental changes, and long-distance transportation. Usually, the laser wavelength is corrected by self-calibration and other methods. The usual self-calibration method is: measure the Raman spectrum of a certain standard substance (such as polystyrene), and compare it with the standard spectrum of the standard substance, and then know the offset of the laser wavelength. The disadvantage of the existing self-calibration method is that it does not have real-time performance, only a constant correction value can be given, and it is difficult to grasp the conditions for self-calibration under what conditions.
发明内容Contents of the invention
本发明的目的是提供一种拉曼光谱检测仪校准方法,本发明提供一种能快速进行进行现场校准的方法。The purpose of the present invention is to provide a method for calibrating a Raman spectroscopic detector, and the present invention provides a method that can quickly perform on-site calibration.
本发明的上述技术目的是通过以下技术方案得以实现的:一种拉曼光谱检测仪校准方法,包括以下操作步骤,The above-mentioned technical purpose of the present invention is achieved through the following technical solutions: a method for calibrating a Raman spectrometer, comprising the following steps,
步骤一,使用拉曼光谱检测仪对标准参考物进行T时间段的信号采样,得到参考光谱S1;Step 1, use the Raman spectrometer to sample the signal of the standard reference substance in the T time period to obtain the reference spectrum S1;
步骤二,使用拉曼光谱检测仪对被待检测物进行所述T时间段的信号采样,得到初始光谱S2;Step 2, using a Raman spectrometer to sample the signal of the substance to be detected in the T time period to obtain an initial spectrum S2;
步骤三,使用拉曼光谱检测仪对空置的样品池进行所述T时间段的信号采样,得到当前背景光谱S3;Step 3, using a Raman spectrometer to sample the signal of the T time period in the empty sample cell to obtain the current background spectrum S3;
步骤四,计算所述参考光谱S1与所述初始光谱S2的第一差值光谱Sd1,计算所述参考光谱S1与当前背景光谱S3的第二差值光谱Sd2,计算所述初始光谱S2与所述当前背景光谱S3的第三差值光谱Sd3;Step 4, calculating the first difference spectrum Sd1 between the reference spectrum S1 and the initial spectrum S2, calculating the second difference spectrum Sd2 between the reference spectrum S1 and the current background spectrum S3, and calculating the difference between the initial spectrum S2 and the Describe the third difference spectrum Sd3 of the current background spectrum S3;
步骤五,分别根据所述第二差值光谱Sd2与所述第三差值光谱Sd3确定参考激光谱峰与被待检物激光谱峰,分别根据所述参考激光谱峰与所述待检物激光谱峰的中心位置分别确定第一偏移量△v1与第二偏移量△v2;Step 5: Determine the reference laser spectrum peak and the laser spectrum peak of the object to be detected according to the second difference spectrum Sd2 and the third difference spectrum Sd3 respectively, and determine the reference laser spectrum peak and the object to be detected according to the The center positions of the laser spectrum peaks respectively determine the first offset Δv1 and the second offset Δv2;
步骤六,比较所述第一偏移量△v1与所述第二偏移量△v2,若相等则采用所述第一偏移量△v1对检测结果的拉曼光谱进行修正;若不相等则根据所述第一差值光谱Sd1确定差值激光谱峰,而后根据所述差值激光谱峰的中心位置确定第三偏移量△v3,使用所述第三偏移量△v3对所述偏移量△v1进行修正得到第四偏移量△v4,最后采用所述第四偏移量△v4对检测结果的拉曼光谱进行修正。Step 6, comparing the first offset Δv1 with the second offset Δv2, if they are equal, use the first offset Δv1 to correct the Raman spectrum of the detection result; if they are not equal Then determine the difference laser spectrum peak according to the first difference spectrum Sd1, then determine the third offset Δv3 according to the center position of the difference laser spectrum peak, and use the third offset Δv3 to determine The above offset Δv1 is corrected to obtain a fourth offset Δv4, and finally the Raman spectrum of the detection result is corrected by using the fourth offset Δv4.
作为本发明的优选,所述步骤五还包括将使用所述第一偏移量△v1对所述标准参考物的检测结果vf直接进行修正,并将修正结果与标准拉曼光谱进行比较后得到第五偏移量△v5,使用所述第五偏移量△v5对所述第一偏移量△v1与所述第二偏移量△v2进行修正得到最终第一偏移量△v1a与最终第二偏移量△v2a,使用所述最终第一偏移量△v1a与所述最终第二偏移量△v2a取代所述第一偏移量△v1与所述第二偏移量△v2后进行步骤六操作。As a preference of the present invention, the step five also includes directly correcting the detection result vf of the standard reference object by using the first offset Δv1, and comparing the correction result with the standard Raman spectrum to obtain The fifth offset Δv5, using the fifth offset Δv5 to correct the first offset Δv1 and the second offset Δv2 to obtain the final first offset Δv1 a and the final second offset Δv2 a , use the final first offset Δv1 a and the final second offset Δv2 a to replace the first offset Δv1 and the second After the offset △v2, proceed to step 6.
作为本发明的优选,所述的拉曼光谱检测仪的陷波滤光片的光密度参数为6.5~7.5。As a preference of the present invention, the optical density parameter of the notch filter of the Raman spectroscopic detector is 6.5-7.5.
作为本发明的优选,还包括在进行所述的步骤一~步骤六的操作之前先置于暗房内预先执行所述步骤一~步骤六进行前置校准。As a preference of the present invention, it also includes placing the method in a darkroom to pre-execute the steps 1 to 6 for pre-calibration before performing the operations of the steps 1 to 6.
作为本发明的优选,所述前置校准的步骤一~步骤六还包括使用标准白炽灯提供背景光进行有光环境初步校准。As a preference of the present invention, the steps 1 to 6 of the pre-calibration further include using a standard incandescent lamp to provide background light for preliminary calibration in a light environment.
作为本发明的优选,当所述第二偏移量△v2为0值时,所述的步骤六中不进行修正直接输出结果。As a preference of the present invention, when the second offset Δv2 has a value of 0, the result is directly output without correction in step six.
作为本发明的优选,当所述第一偏移量△v1为0值时,所述步骤六中直接使用所述第二偏移量△v2对检测结果的拉曼光谱进行修正。As a preference of the present invention, when the first offset Δv1 is 0, the second offset Δv2 is directly used in the step 6 to correct the Raman spectrum of the detection result.
作为本发明的优选,所述的标准参考物为聚苯乙烯。As a preference of the present invention, said standard reference substance is polystyrene.
综上所述,本发明具有如下有益效果:In summary, the present invention has the following beneficial effects:
本发明拥有校准参照多,校准度高,实时性好的优点。The invention has the advantages of many calibration references, high calibration degree and good real-time performance.
附图说明Description of drawings
图1是本发明的实施例的操作流程图。FIG. 1 is a flowchart of the operation of an embodiment of the present invention.
具体实施方式Detailed ways
以下结合附图对本发明作进一步详细说明。The present invention will be described in further detail below in conjunction with the accompanying drawings.
如图1所示,本发明的第一种实施例包括以下操作步骤,As shown in Figure 1, the first embodiment of the present invention includes the following steps,
步骤一,使用拉曼光谱检测仪对标准参考物进行标准的统一测试时间T时间段的信号采样,得到参考光谱S1,其中标准参考物为聚苯乙烯,拉曼光谱检测仪的陷波滤光片的光密度参数为6.5~7.5;Step 1, use the Raman spectroscopic detector to sample the signal of the standard unified test time T time period on the standard reference substance to obtain the reference spectrum S1, wherein the standard reference substance is polystyrene, and the notch filter of the Raman spectroscopic detector The optical density parameter of the sheet is 6.5-7.5;
步骤二,使用拉曼光谱检测仪对被待检测物进行T时间段的信号采样,得到初始光谱S2;Step 2, use the Raman spectrometer to sample the signal of the substance to be detected in the T time period to obtain the initial spectrum S2;
步骤三,使用拉曼光谱检测仪对空置的样品池进行T时间段的信号采样,得到当前背景光谱S3;Step 3, use the Raman spectrometer to sample the signal of the empty sample pool for a time period of T to obtain the current background spectrum S3;
步骤四,计算参考光谱S1与初始光谱S2的第一差值光谱Sd1,计算参考光谱S1与当前背景光谱S3的第二差值光谱Sd2,计算初始光谱S2与当前背景光谱S3的第三差值光谱Sd3;Step 4: Calculate the first difference spectrum Sd1 between the reference spectrum S1 and the initial spectrum S2, calculate the second difference spectrum Sd2 between the reference spectrum S1 and the current background spectrum S3, and calculate the third difference between the initial spectrum S2 and the current background spectrum S3 Spectrum Sd3;
步骤五,分别根据第二差值光谱Sd2与第三差值光谱Sd3确定参考激光谱峰与被待检物激光谱峰,分别根据参考激光谱峰与待检物激光谱峰的中心位置分别确定两次采样过程中激光波长相对拉曼光谱检测仪给出的参考激光波长之间的第一偏移量△v1与第二偏移量△v2;Step 5: Determine the reference laser spectrum peak and the laser spectrum peak of the object to be detected according to the second difference spectrum Sd2 and the third difference spectrum Sd3 respectively, and determine respectively according to the center positions of the reference laser spectrum peak and the laser spectrum peak of the object to be detected The first offset △v1 and the second offset △v2 between the laser wavelength and the reference laser wavelength given by the Raman spectrometer during the two sampling processes;
步骤六,比较第一偏移量△v1与第二偏移量△v2,若相等则采用第一偏移量△v1对检测结果vi的拉曼光谱进行修正,修正方式为vi=vi+△v1;若不相等则根据第一差值光谱Sd1确定差值激光谱峰,而后根据差值激光谱峰的中心位置确定参考物采样过程中激光波长相对被检物采样过程中激光波长之间的第三偏移量△v3,使用第三偏移量△v3对偏移量△v1进行修正得到第四偏移量△v4,最后采用第四偏移量△v4对检测结果的拉曼光谱进行修正,修正方式为vi=vi+△v4,本步骤中当第二偏移量△v2为0值时,步骤六中不进行修正直接输出结果。当第一偏移量△v1为0值时,步骤六中直接使用第二偏移量△v2对检测结果vi的拉曼光谱进行修正。Step 6, compare the first offset △v1 and the second offset △v2, if they are equal, use the first offset △v1 to correct the Raman spectrum of the detection result vi, the correction method is vi=vi+△v1 If not equal, then determine the difference laser spectrum peak according to the first difference spectrum Sd1, and then determine the second laser wavelength between the laser wavelength in the sampling process of the reference object relative to the laser wavelength in the sampling process of the tested object according to the center position of the difference laser spectrum peak Three offsets △v3, use the third offset △v3 to correct the offset △v1 to get the fourth offset △v4, and finally use the fourth offset △v4 to correct the Raman spectrum of the detection result , the correction method is vi=vi+Δv4. In this step, when the second offset Δv2 is 0, the result is directly output without correction in step six. When the first offset Δv1 is 0, the second offset Δv2 is directly used in step 6 to correct the Raman spectrum of the detection result vi.
本发明的第二种实施例在保持第一种实施例的全部操作步骤的前提下在步骤五重增加操作,该操作方法为将使用第一偏移量△v1对标准参考物的检测结果vf直接进行修正,并将修正结果与标准拉曼光谱进行比较,标准拉曼光谱为理论上聚苯乙烯的标准拉曼光谱,比较后得到第五偏移量△v5,使用第五偏移量△v5对第一偏移量△v1与第二偏移量△v2进行修正得到最终第一偏移量△v1a与最终第二偏移量△v2a,使用最终第一偏移量△v1a与最终第二偏移量△v2a取代第一偏移量△v1与第二偏移量△v2后进行步骤六操作。In the second embodiment of the present invention, on the premise of keeping all the operation steps of the first embodiment, the operation is added in the fifth step. The operation method is to use the first offset Δv1 to the detection result vf of the standard reference object Perform the correction directly, and compare the correction result with the standard Raman spectrum. The standard Raman spectrum is the standard Raman spectrum of polystyrene in theory. After comparison, the fifth offset △v5 is obtained, and the fifth offset △ v5 corrects the first offset △v1 and the second offset △v2 to obtain the final first offset △v1 a and the final second offset △v2 a , using the final first offset △v1 a Step 6 is performed after replacing the first offset Δv1 and the second offset Δv2 with the final second offset Δv2 a .
本发明实施例一与实施例二在进行步骤一~步骤六的操作之前先置于暗房内预先执行步骤一~步骤六进行前置校准,前置校准的目的是为了在日常检测前消除出厂出现的误差,前置校准必须保证△v1~△v5均为0值。前置校准的步骤一~步骤六还包括使用经过积分球进行光参数测试并达到标准光源要求的标准白炽灯提供背景光进行有光环境初步校准,这一步骤为了产生一个标准光环境下的偏移量进行出厂的有光环境校准。Embodiment 1 and Embodiment 2 of the present invention are placed in the darkroom before performing steps 1 to 6 for pre-calibration. The purpose of pre-calibration is to eliminate the occurrence The pre-calibration must ensure that △v1~△v5 are all 0 values. Steps 1 to 6 of the pre-calibration also include the use of a standard incandescent lamp that has been tested for light parameters by an integrating sphere and meets the requirements of a standard light source to provide background light for preliminary calibration in a light environment. The factory light environment calibration is carried out by shift amount.
本具体实施例仅仅是对本发明的解释,其并不是对本发明的限制,本领域技术人员在阅读完本说明书后可以根据需要对本实施例做出没有创造性贡献的修改,但只要在本发明的权利要求范围内都受到专利法的保护。This specific embodiment is only an explanation of the present invention, and it is not a limitation of the present invention. Those skilled in the art can make modifications to this embodiment without creative contribution as required after reading this specification, but as long as they are within the rights of the present invention All claims are protected by patent law.
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